Resolved Specific Ion Data Collections

Temperature Range
8.341 eV → 8.341 x 104 eV


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  • Spontaneous Emission: Fe+21(i) → Fe+21(j) + hv
  • Electron Impact Excitation: Fe+21(i) + e → Fe+21(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 118266.0 cm-1
2s1 2p2 4P0.5 404550.0 cm-1
2s1 2p2 4P1.5 460190.0 cm-1
2s1 2p2 4P2.5 513260.0 cm-1
2s1 2p2 2D1.5 736310.0 cm-1
2s1 2p2 2D2.5 759210.0 cm-1
2s1 2p2 2P0.5 853650.0 cm-1
2s1 2p2 2S0.5 978350.0 cm-1
2s1 2p2 2P1.5 992320.0 cm-1
2p3 4S1.5 1255700.0 cm-1
2p3 2D1.5 1396110.0 cm-1
2p3 2D2.5 1426570.0 cm-1
2p3 2P0.5 1569630.0 cm-1
2p3 2P1.5 1627720.0 cm-1
2s2 3s1 2S0.5 8127280.0 cm-1
2s2 3p1 2P0.5 8307720.0 cm-1
2s2 3p1 2P1.5 8340230.0 cm-1
2s1 2p1 3s1 4P0.5 8485530.0 cm-1
2s2 3d1 2D1.5 8508170.0 cm-1
2s1 2p1 3s1 4P1.5 8516150.0 cm-1
2s2 3d1 2D2.5 8518640.0 cm-1
2s1 2p1 3s1 2P0.5 8584300.0 cm-1
2s1 2p1 3s1 4P2.5 8596160.0 cm-1
2s1 2p1 3p1 4D0.5 8645350.0 cm-1
2s1 2p1 3s1 2P1.5 8669830.0 cm-1
2s1 2p1 3p1 4D1.5 8672680.0 cm-1
2s1 2p1 3p1 2P1.5 8708150.0 cm-1
2s1 2p1 3p1 2P0.5 8717140.0 cm-1
2s1 2p1 3p1 4D2.5 8721260.0 cm-1
2s1 2p1 3p1 4P0.5 8740360.0 cm-1
2s1 2p1 3p1 2D1.5 8760320.0 cm-1
2s1 2p1 3p1 4D3.5 8793390.0 cm-1
2s1 2p1 3p1 4P1.5 8799690.0 cm-1
2s1 2p1 3p1 4P2.5 8816940.0 cm-1
2s1 2p1 3p1 4S1.5 8819440.0 cm-1
2s1 2p1 3d1 4F1.5 8827380.0 cm-1
2s1 2p1 3d1 4F2.5 8847080.0 cm-1
2s1 2p1 3p1 2D2.5 8865270.0 cm-1
2s1 2p1 3d1 4F3.5 8878100.0 cm-1
2s1 2p1 3d1 4P2.5 8889990.0 cm-1
2s1 2p1 3p1 2S0.5 8896680.0 cm-1
2s1 2p1 3d1 4D1.5 8898880.0 cm-1
2s1 2p1 3s1 2P0.5 8899030.0 cm-1
2s1 2p1 3s1 2P1.5 8902230.0 cm-1
2s1 2p1 3d1 4D0.5 8903070.0 cm-1
2s1 2p1 3d1 2D1.5 8934800.0 cm-1
2s1 2p1 3d1 4F4.5 8941740.0 cm-1
2s1 2p1 3d1 2D2.5 8950390.0 cm-1
2s1 2p1 3d1 4D3.5 8972660.0 cm-1
2s1 2p1 3d1 4D2.5 8983070.0 cm-1
2s1 2p1 3d1 4P1.5 8987240.0 cm-1
2s1 2p1 3d1 4P0.5 8989130.0 cm-1
2s1 2p1 3d1 2F2.5 9023610.0 cm-1
2s1 2p1 3d1 2P1.5 9060930.0 cm-1
2s1 2p1 3p1 2P0.5 9078380.0 cm-1
2s1 2p1 3d1 2F3.5 9079930.0 cm-1
2s1 2p1 3p1 2D1.5 9085110.0 cm-1
2s1 2p1 3d1 2P0.5 9094870.0 cm-1
2s1 2p1 3p1 2D2.5 9105130.0 cm-1
2s1 2p1 3p1 2P1.5 9113170.0 cm-1
2p2 3s1 4P0.5 9129170.0 cm-1
2s1 2p1 3p1 2S0.5 9162500.0 cm-1
2p2 3s1 4P1.5 9198320.0 cm-1
2p2 3s1 4P2.5 9245540.0 cm-1
2p2 3s1 2P0.5 9264010.0 cm-1
2s1 2p1 3d1 2F3.5 9269260.0 cm-1
2s1 2p1 3d1 2F2.5 9270730.0 cm-1
2p2 3p1 4D0.5 9279650.0 cm-1
2s1 2p1 3d1 2D1.5 9281830.0 cm-1
2s1 2p1 3d1 2D2.5 9295280.0 cm-1
2p2 3s1 2P1.5 9303610.0 cm-1
2s1 2p1 3d1 2P0.5 9316500.0 cm-1
2s1 2p1 3d1 2P1.5 9318220.0 cm-1
2p2 3p1 4D1.5 9333410.0 cm-1
2p2 3p1 2S0.5 9336200.0 cm-1
2p2 3p1 4P1.5 9372730.0 cm-1
2p2 3p1 4D2.5 9380870.0 cm-1
2p2 3s1 2D2.5 9390400.0 cm-1
2p2 3p1 4P0.5 9397020.0 cm-1
2p2 3p1 4P2.5 9402940.0 cm-1
2p2 3s1 2D1.5 9408660.0 cm-1
2p2 3p1 2D1.5 9418110.0 cm-1
2p2 3p1 4D3.5 9427880.0 cm-1
2p2 3d1 4F1.5 9459710.0 cm-1
2p2 3p1 4S1.5 9475050.0 cm-1
2p2 3p1 2D2.5 9484380.0 cm-1
2p2 3d1 4F2.5 9484610.0 cm-1
2p2 3p1 2P1.5 9485910.0 cm-1
2p2 3p1 2P0.5 9514600.0 cm-1
2p2 3d1 4F3.5 9529900.0 cm-1
2p2 3d1 2P1.5 9530860.0 cm-1
2p2 3d1 4D0.5 9538070.0 cm-1
2p2 3d1 4D2.5 9538710.0 cm-1
2p2 3p1 2F2.5 9558330.0 cm-1
2p2 3d1 4D3.5 9567060.0 cm-1
2p2 3d1 4F4.5 9569760.0 cm-1
2p2 3d1 4D1.5 9570650.0 cm-1
2p2 3d1 2F2.5 9573480.0 cm-1
2p2 3p1 2F3.5 9574220.0 cm-1
2p2 3p1 2D1.5 9595350.0 cm-1
2p2 3s1 2S0.5 9606980.0 cm-1
2p2 3p1 2D2.5 9611390.0 cm-1
2p2 3d1 4P2.5 9616340.0 cm-1
2p2 3p1 2P0.5 9625230.0 cm-1
2p2 3d1 4P1.5 9629940.0 cm-1
2p2 3d1 2P0.5 9632200.0 cm-1
2p2 3d1 4P0.5 9639770.0 cm-1
2p2 3d1 2F3.5 9644880.0 cm-1
2p2 3d1 2D2.5 9687130.0 cm-1
2p2 3d1 2D1.5 9689030.0 cm-1
2p2 3p1 2P1.5 9694700.0 cm-1
2p2 3d1 2G3.5 9703420.0 cm-1
2p2 3d1 2G4.5 9720880.0 cm-1
2p2 3d1 2D1.5 9746410.0 cm-1
2p2 3d1 2D2.5 9753170.0 cm-1
2p2 3d1 2P0.5 9776930.0 cm-1
2p2 3d1 2F3.5 9778180.0 cm-1
2p2 3p1 2P0.5 9795390.0 cm-1
2p2 3p1 2P1.5 9814150.0 cm-1
2p2 3d1 2F2.5 9814980.0 cm-1
2p2 3d1 2S0.5 9815200.0 cm-1
2p2 3d1 2P1.5 9819020.0 cm-1
2p2 3d1 2D2.5 9968440.0 cm-1
2p2 3d1 2D1.5 9976600.0 cm-1
2s2 4s1 2S0.5 11018000.0 cm-1
2s2 4p1 2P0.5 11092400.0 cm-1
2s2 4p1 2P1.5 11105800.0 cm-1
2s2 4d1 2D1.5 11167500.0 cm-1
2s2 4d1 2D2.5 11171800.0 cm-1
2s2 4f1 2F2.5 11207800.0 cm-1
2s2 4f1 2F3.5 11209800.0 cm-1
2s1 2p1 4s1 4P0.5 11371400.0 cm-1
2s1 2p1 4s1 4P1.5 11400000.0 cm-1
2s1 2p1 4s1 2P0.5 11420000.0 cm-1
2s1 2p1 4p1 4D0.5 11437900.0 cm-1
2s1 2p1 4p1 4D1.5 11457700.0 cm-1
2s1 2p1 4p1 4S1.5 11469700.0 cm-1
2s1 2p1 4s1 4P2.5 11482300.0 cm-1
2s1 2p1 4p1 4P0.5 11485900.0 cm-1
2s1 2p1 4p1 4D2.5 11486600.0 cm-1
2s1 2p1 4p1 2P0.5 11489700.0 cm-1
2s1 2p1 4p1 2D1.5 11499800.0 cm-1
2s1 2p1 4s1 2P1.5 11506500.0 cm-1
2s1 2p1 4d1 4F1.5 11509600.0 cm-1
2s1 2p1 4d1 4F2.5 11521200.0 cm-1
2s1 2p1 4d1 4P2.5 11541900.0 cm-1
2s1 2p1 4d1 4F3.5 11547600.0 cm-1
2s1 2p1 4d1 4D1.5 11549300.0 cm-1
2s1 2p1 4d1 4D0.5 11552200.0 cm-1
2s1 2p1 4f1 4G2.5 11555200.0 cm-1
2s1 2p1 4f1 4D3.5 11557700.0 cm-1
2s1 2p1 4p1 4P1.5 11562600.0 cm-1
2s1 2p1 4p1 4D3.5 11564100.0 cm-1
2s1 2p1 4d1 2D1.5 11564800.0 cm-1
2s1 2p1 4p1 4P2.5 11566300.0 cm-1
2s1 2p1 4d1 2F2.5 11572000.0 cm-1
2s1 2p1 4p1 2P1.5 11573600.0 cm-1
2s1 2p1 4f1 4F1.5 11583600.0 cm-1
2s1 2p1 4f1 4G3.5 11585200.0 cm-1
2s1 2p1 4f1 4D2.5 11585600.0 cm-1
2s1 2p1 4f1 4G4.5 11586100.0 cm-1
2s1 2p1 4p1 2D2.5 11588800.0 cm-1
2s1 2p1 4f1 2F2.5 11592600.0 cm-1
2s1 2p1 4f1 2G3.5 11592700.0 cm-1
2s1 2p1 4p1 2S0.5 11601300.0 cm-1
2s1 2p1 4d1 4F4.5 11622600.0 cm-1
2s1 2p1 4d1 4D3.5 11630100.0 cm-1
2s1 2p1 4d1 4D2.5 11633100.0 cm-1
2s1 2p1 4d1 4P1.5 11636000.0 cm-1
2s1 2p1 4d1 4P0.5 11637000.0 cm-1
2s1 2p1 4d1 2D2.5 11646000.0 cm-1
2s1 2p1 4d1 2P1.5 11657100.0 cm-1
2s1 2p1 4d1 2F3.5 11666400.0 cm-1
2s1 2p1 4f1 4F3.5 11669200.0 cm-1
2s1 2p1 4f1 4F4.5 11669600.0 cm-1
2s1 2p1 4f1 4F2.5 11671300.0 cm-1
2s1 2p1 4d1 2P0.5 11671900.0 cm-1
2s1 2p1 4f1 2F3.5 11673900.0 cm-1
2s1 2p1 4f1 4G5.5 11674000.0 cm-1
2s1 2p1 4f1 4D1.5 11675300.0 cm-1
2s1 2p1 4f1 4D0.5 11678100.0 cm-1
2s1 2p1 4f1 2G4.5 11678500.0 cm-1
2s1 2p1 4f1 2D2.5 11678600.0 cm-1
2s1 2p1 4f1 2D1.5 11684600.0 cm-1
2s1 2p1 4s1 2P0.5 11777600.0 cm-1
2s1 2p1 4s1 2P1.5 11779200.0 cm-1
2s1 2p1 4p1 2D1.5 11850200.0 cm-1
2s1 2p1 4p1 2P0.5 11851800.0 cm-1
2s1 2p1 4p1 2D2.5 11859500.0 cm-1
2s1 2p1 4p1 2P1.5 11865000.0 cm-1
2s1 2p1 4p1 2S0.5 11874500.0 cm-1
2s1 2p1 4d1 2D1.5 11923200.0 cm-1
2s1 2p1 4d1 2F2.5 11923700.0 cm-1
2s1 2p1 4d1 2F3.5 11924100.0 cm-1
2s1 2p1 4d1 2D2.5 11928600.0 cm-1
2s1 2p1 4d1 2P0.5 11937000.0 cm-1
2s1 2p1 4d1 2P1.5 11941300.0 cm-1
2s1 2p1 4f1 2F2.5 11953600.0 cm-1
2s1 2p1 4f1 2F3.5 11955600.0 cm-1
2s1 2p1 4f1 2G3.5 11964000.0 cm-1
2s1 2p1 4f1 2G4.5 11965800.0 cm-1
2s1 2p1 4f1 2D1.5 11970400.0 cm-1
2s1 2p1 4f1 2D2.5 11972200.0 cm-1

        Result of ICFT R-matrix calculation

 Calculation automated by offline ADAS code ADAS8#3

     Summary Information

 *  Ionisation energy taken from ADAS adf00 files

 *  Energy levels calculated by AUTOSTRUCTURE

 *  Radiative rates calculated by AUTOSTRUCTURE

 *  Effective collision strengths calculated by ICFT
    R-matrix calculation using target structure from

     Calculation details

 The following scaling parameters on bound orbitals were used:

         1S = 1.37933
         2S = 1.25161
         2P = 1.17515
         3S = 1.58174
         3P = 1.37353
         3D = 1.48629
         4S = 1.50142
         4P = 1.38397
         4D = 1.53745
         4F = 1.57746

 An exchange calculation was performed up to J=12
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 1581.8916 Rydbergs (21523.217110 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.06000246 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.000246 eV) was used
 from the last threshold up to 0.899468 Z**2 Rydbergs (5397.0318 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.000246 eV) was used
 from first threshold up to 0.899468 Z**2 Rydbergs (5397.0318 eV) in the
 non-exchange calculation.

 Dipole and Born limits were used from the last calculated energy points
 up to infinite energy to complete the effective collision strengths

      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        08/11/11


  • Guiyun Liang
  • Nigel Badnell
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